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In a bent member, normal stress varies linearly with distance from the neutral axis. At the neutral axis, stress is zero. Stress increases proportionally as you move toward the outer fibers. This linear relationship applies within the elastic limit and is described by the flexural stress formula, which relates stress to the bending moment, moment of inertia, and distance from the neutral axis.

When analyzing force equilibrium in a bent member, the sum of longitudinal forces must equal zero. Since stress varies linearly from the neutral axis and integrates to zero across the section, the neutral axis must coincide with the centroid. This geometric relationship ensures that tensile and compressive stresses balance, confirming the neutral axis location at the section's centroid.

Hooke's Law establishes that stress is proportional to strain within the elastic limit. In bending, strain varies linearly from zero at the neutral axis to maximum at the outer fibers. Multiplying strain by the modulus of elasticity yields the normal stress distribution. This relationship is fundamental to connecting the bending moment to the resulting stress through the flexural stress formula.

The moment of inertia of the cross-section with respect to the centroidal axis appears in the flexural stress formula's denominator. It quantifies how the cross-sectional area is distributed relative to the neutral axis. A larger moment of inertia reduces flexural stress for the same bending moment, making it a critical geometric property in predicting how members resist bending and experience stress.

The flexural stress formula calculates the normal stress at any distance from the neutral axis in a bent member. It combines the bending moment, moment of inertia, and distance from the neutral axis to determine stress magnitude. Maximum stress occurs at the outermost fibers. This formula applies to symmetric members within elastic limits and is essential for designing members to withstand bending loads.

Strain varies linearly from zero at the neutral axis to maximum at the outer fibers, proportional to distance from the neutral axis. When multiplied by the modulus of elasticity through Hooke's Law, this linear strain distribution produces a corresponding linear stress distribution. The maximum strain at distance 'c' from the neutral axis directly determines the maximum flexural stress in the member.

The flexural stress formula and its derivation depend on Hooke's Law, which only applies within the elastic limit where stress is proportional to strain. Beyond this limit, material behavior becomes nonlinear and the linear relationships break down. Assuming elastic behavior ensures the formula accurately predicts stress distribution and allows engineers to design members safely within material limits.